Search results for "medium"

showing 10 items of 3746 documents

Blue luminescence in ZnO single crystals, nanopowders, ceramic

2007

The luminescence spectra and luminescence decay processes were studied in a ZnO single crystal, nanopowders and ceramic at liquid helium and room temperature under VUV synchrotron radiation as well as under pulsed laser excitation. The exciton-exciton and exciton-multiphonon processes were compared in different ZnO nanopowders (commercial powder, powders obtained by vaporization-condensation technique) and ceramic. The possibility of luminescence decay time modification by Al3+ doping was shown.

Condensed Matter::Quantum GasesHistoryMaterials scienceCondensed Matter::Otherbusiness.industryLiquid heliumDopingSynchrotron radiationLuminescence spectraComputer Science ApplicationsEducationlaw.inventionCondensed Matter::Materials SciencelawCondensed Matter::Superconductivityvisual_artPhysics::Atomic and Molecular Clustersvisual_art.visual_art_mediumOptoelectronicsddc:530CeramicLuminescencebusinessSingle crystalExcitationJournal of Physics: Conference Series
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Colossal Density-Driven Resistance Response in the Negative Charge Transfer Insulator MnS2

2021

A reversible density driven insulator to metal to insulator transition in high-spin MnS_{2} is experimentally observed, leading with a colossal electrical resistance drop of 10^{8}  Ω by 12 GPa. Density functional theory simulations reveal the metallization to be unexpectedly driven by previously unoccupied S_{2}^{2-} σ_{3p}^{*} antibonding states crossing the Fermi level. This is a unique variant of the charge transfer insulator to metal transition for negative charge transfer insulators having anions with an unsaturated valence. By 36 GPa the emergence of the low-spin insulating arsenopyrite (P2_{1}/c) is confirmed, and the bulk metallicity is broken with the system returning to an insula…

Condensed Matter::Quantum GasesMaterials scienceValence (chemistry)Condensed matter physicsFermi levelGeneral Physics and AstronomyInsulator (electricity)Charge (physics)Antibonding molecular orbitalMetalCondensed Matter::Materials Sciencesymbols.namesakeElectrical resistance and conductancevisual_artsymbolsvisual_art.visual_art_mediumCondensed Matter::Strongly Correlated ElectronsDensity functional theoryPhysical Review Letters
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Trapping and mobilization of residual fluid during capillary desaturation in porous media

1998

We discuss the problem of trapping and mobilization of nonwetting fluids during immiscible two-phase displacement processes in porous media. Capillary desaturation curves give residual saturations as a function of capillary number. Interpreting capillary numbers as the ratio of viscous to capillary forces the breakpoint in experimental curves contradicts the theoretically predicted force balance. We show that replotting the data against a novel macroscopic capillary number resolves the problem for discontinuous mode displacement.

Condensed Matter::Soft Condensed MatterPhysics::Fluid DynamicsCapillary pressureMaterials scienceCapillary actionTrappingMechanicsResidualGranular materialPorous mediumDisplacement (fluid)Capillary numberPhysical Review E
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New BEDT-TTF/[Fe(C5O5)3]3- Hybrid System:  Synthesis, Crystal Structure, and Physical Properties of a Chirality-Induced α Phase and a Novel Magnetic …

2007

The paramagnetic and chiral anion [Fe(C5O5)3]3- (C5O52-=croconate) has been combined with the organic donor BEDT-TTF (=ET=bis(ethylenedithio)tetrathiafulvalene) to synthesize a novel paramagnetic semiconductor with the first chirality-induced alpha phase, alpha-(BEDT-TTF)5[Fe(C5O5)3].5H2O (1), and one of the few known paramagnetic molecular metals, beta-(BEDT-TTF)5[Fe(C5O5)3].C6H5CN (2). Both compounds present layers of BEDT-TTF molecules, with the alpha or beta packing modes, alternating with layers containing the high-spin S=5/2 Fe(III) anions and solvent molecules. In the alpha phase, the alternation of the chiral [Fe(C5O5)3]3- anions along the direction perpendicular to the BEDT-TTF cha…

Condensed matter physicsCharge densityCrystal structureConductivityIonInorganic ChemistryMetalParamagnetismchemistry.chemical_compoundCrystallographychemistryvisual_artvisual_art.visual_art_mediumPhysical and Theoretical ChemistryElectronic band structureTetrathiafulvaleneInorganic Chemistry
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Adatom Island Diffusion on Metal Fcc(100) Surfaces

2001

We study the energetics and atomic mechanisms of diffusion of adatom islands on fcc(100) metal surfaces. For small islands, we perform detailed microscopic calculations using semi-empirical embedded-atom model and glue potentials in the case of Cu and Al, respectively. Combining systematic saddle-point search methods and molecular statics simulations allows us to find all the relevant transition paths for island motion. In particular, we demonstrate that there are novel many-body mechanisms such as internal row shearing which can, in some cases, control the island dynamics. Next, we show how using the master equation formalism, diffusion coefficients for small islands up to about five atoms…

Condensed matter physicsChemistryMonte Carlo methodCrossoverEnergeticsMolecular statics02 engineering and technology021001 nanoscience & nanotechnology01 natural sciencesMetalvisual_art0103 physical sciencesMaster equationvisual_art.visual_art_mediumKinetic Monte Carlo010306 general physics0210 nano-technologySaddle
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Spin crossover in a tetranuclear Cr(III)-Fe(III)3 complex

2004

A novel heteronuclear exchange-coupled complex [Cr I I I {(CN)Fe I I I -( 5 L)} 3 (CN) 3 ] containing a pentadentate blocking ligand 5 L was synthesized. The X-ray structure shows that a meridional isomer applies with inequivalent Fe I I I centers. The complex exhibits a thermally induced spin crossover along with the exchange coupling. Mossbauer spectra indicate a spin transition between S = ½ and S = 5/2 states although a considerable amount of Fe I I I centers stays high-spin at T = 6 K. The magnetization, the magnetic susceptibility, and the Mossbauer data were fitted in one run with a spin crossover model taking into account exchange interactions among all metal centers.

Condensed matter physicsChemistrySpin transitionZonal and meridionalMagnetic susceptibilityInorganic ChemistryMetalMagnetizationCrystallographyHeteronuclear moleculeSpin crossovervisual_artMössbauer spectroscopyvisual_art.visual_art_mediumPhysical and Theoretical Chemistry
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Semiconducting half-Heusler and LiGaGe structure type compounds

2009

Compounds with LiAlSi (half-Heusler) and LiGaGe structure types have been investigated by means of band structure calculations. The LiAlSi structure type is known as the half-Heusler structure type, whereas LiGaGe is a closely related hexagonal variant. A remarkable feature of some XYZ half-Heusler compounds with 8 and 18 valence electrons is, that despite being composed of only metallic elements, they are semiconductors. More than 100 semiconducting compounds within these structure types are known. LiGaGe compounds have an additional degree of freedom, namely the degree of puckering of the layers. These compounds can become semiconducting at a certain degree of puckering. Half-metallic beh…

Condensed matter physicsbusiness.industryChemistryHexagonal crystal systemSurfaces and InterfacesStructure typeElectronic density of statesCondensed Matter PhysicsSemimetalSurfaces Coatings and FilmsElectronic Optical and Magnetic MaterialsMetalSemiconductorvisual_artMaterials Chemistryvisual_art.visual_art_mediumElectrical and Electronic EngineeringbusinessValence electronElectronic band structurephysica status solidi (a)
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Biochemical Applications of Solid Supported Membranes on Gold Surfaces: Quartz Crystal Microbalance and Impedance Analysis

2003

Since their inception in 1985 by Tamm and McConnell [1], solid supported lipid bilayers have been widely used as model systems for cellular membranes [2]. They have been applied in fundamental and applied studies of lipid assemblies on surfaces, to study the structure of membranes and membrane dynamics, lipidreceptor-interactions and electrochemical properties of membranes [3-5]. Several attempts have been made to apply solid supported membranes (SSM) in biosensor devices [6]. Planar lipid membranes can be formed on various surfaces, i.e. glass, silicon, mica or metal surfaces such as platinum or gold. Surface attachment of the lipids is typically achieved following two different strategies…

Conductive polymerMaterials scienceSiliconOxidechemistry.chemical_elementQuartz crystal microbalanceMetalchemistry.chemical_compoundMembranechemistryChemical engineeringvisual_artvisual_art.visual_art_mediumLipid bilayerBiosensor
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Intrinsic electrical conductivity of nanostructured metal-organic polymer chains

2012

One-dimensional conductive polymers are attractive materials because of their potential in flexible and transparent electronics. Despite years of research, on the macro- and nano-scale, structural disorder represents the major hurdle in achieving high conductivities. Here we report measurements of highly ordered metal-organic nanoribbons, whose intrinsic (defect-free) conductivity is found to be 104 S m−1, three orders of magnitude higher than that of our macroscopic crystals. This magnitude is preserved for distances as large as 300 nm. Above this length, the presence of structural defects (~ 0.5%) gives rise to an inter-fibre-mediated charge transport similar to that of macroscopic crysta…

Conductive polymerMultidisciplinaryMaterials scienceOrders of magnitude (temperature)General Physics and AstronomyNanotechnologyGeneral ChemistryElectronic structureConductivityArticleGeneral Biochemistry Genetics and Molecular BiologyMetalMolecular wireGapless playbackChemical physicsElectrical resistivity and conductivityvisual_artvisual_art.visual_art_mediumNature Communications
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Large time behavior for a porous medium equation in a nonhomogeneous medium with critical density

2014

Abstract We study the large time behavior of solutions to the Cauchy problem for the porous medium equation in nonhomogeneous media with critical singular density | x | − 2 ∂ t u = Δ u m , in R N × ( 0 , ∞ ) , where m > 1 and N ≥ 3 , with nonnegative initial condition u ( x , 0 ) = u 0 ( x ) ≥ 0 . The asymptotic behavior proves to have some interesting and striking properties. We show that there are different asymptotic profiles for the solutions, depending on whether the continuous initial data u 0 vanishes at x = 0 or not. Moreover, when u 0 ( 0 ) = 0 , we show the convergence towards a peak-type profile presenting a jump discontinuity, coming from an interesting asymptotic simplification…

Conservation lawSingularityApplied MathematicsMathematical analysisConvergence (routing)Initial value problemScale (descriptive set theory)Limit (mathematics)Classification of discontinuitiesPorous mediumAnalysisMathematicsNonlinear Analysis: Theory, Methods & Applications
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